2 research outputs found

    Probing axion-like particles with γγ\gamma \gamma final states from vector boson fusion processes at the LHC

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    We perform a feasibility study to search for axion-like particles (ALPs) using vector boson fusion (VBF) processes at the LHC. We work in an effective field theory framework with cutoff scale Λ\Lambda and ALP mass mam_{a}, and assume that ALPs couple to photons with strength 1/Λ\propto 1/\Lambda. Assuming proton-proton collisions at s=13\sqrt{s} = 13 TeV, we present the total VBF ALP production cross sections, ALP decay widths and lifetimes, and relevant kinematic distributions as a function of mam_{a} and Λ\Lambda. We consider the aγγa\to\gamma\gamma decay mode to show that the requirement of an energetic diphoton pair combined with two forward jets with large dijet mass and pseudorapidity separation can significantly reduce the Standard Model backgrounds, leading to a 5σ5\sigma discovery reach for 10 MeVma110 \text{ MeV} \lesssim m_{a} \lesssim 1 TeV with Λ2\Lambda \lesssim 2 TeV, assuming an integrated luminosity of 3000 fb1^{-1}. In particular, this extends the LHC sensitivity to a previously unstudied region of the ALP parameter space.Comment: 9 pages, 5 figure

    The Pixel Luminosity Telescope: a detector for luminosity measurement at CMS using silicon pixel sensors

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    International audienceThe Pixel Luminosity Telescope is a silicon pixel detector dedicated to luminosity measurement at the CMS experiment at the LHC. It is located approximately 1.75 m from the interaction point and arranged into 16 “telescopes”, with eight telescopes installed around the beam pipe at either end of the detector and each telescope composed of three individual silicon sensor planes. The per-bunch instantaneous luminosity is measured by counting events where all three planes in the telescope register a hit, using a special readout at the full LHC bunch-crossing rate of 40 MHz. The full pixel information is read out at a lower rate and can be used to determine calibrations, corrections, and systematic uncertainties for the online and offline measurements. This paper details the commissioning, operational history, and performance of the detector during Run 2 (2015–18) of the LHC, as well as preparations for Run 3, which will begin in 2022
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